Different values for the inertia of a moving object?

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The discussion centers on the misconception that relativity requires different inertia values for moving objects in different directions, which contradicts the principle of isotropy in physics. It emphasizes that the laws of physics remain consistent across all directions, and any perceived discrepancies arise from human choices in coordinate systems rather than fundamental laws. The use of 4-vectors is suggested as a more effective approach, eliminating the need for distinguishing between transverse and longitudinal relativistic mass. The conversation also critiques outdated concepts found in older literature and highlights the importance of simplifying definitions in physics. Overall, the thread clarifies that relativity does not imply varying inertia based on motion direction.
csmcmillion
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I would appreciate terse responses to the following statement:

"Relativity requires different values for the inertia of a moving object: in its direction of motion, and perpendicular to that direction. This contradicts the logical principle that the laws of physics are the same in all directions."

Thanks.
 
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Relativity says that when you transform into a frame in which you are standing still, space has the same properties in all directions. Which is true, and necessary for isotropy.

A lot of people assume that if you have all the laws of physics, the Newtonian laws apply without any modification. This is incorrect and a source of confusion.

Another way of saying this is that the statement is not a statement about the laws of physics, but about human choices, coordinate choices. If it were about the laws of physics, there would be some sort of experiment that tells you which frame is moving, and which isn't. But the point of relativity is that there isn't.
 
To add to Pervect, the idea of transverse and longitudinal relativistic mass derives from the choice to use F=ma, where 'a' is spatial acceleration. To my mind, this is as silly as trying to come up with compensations to mechanics such that you can use normal velocity addition in SR rather than relativistic velocity addition.

If, instead, you use 4-vectors, you have:

p = m U (U being 4-velocity)

and

F = dp/d tau (F now being 4 force)

with no need for any transverse and longitudinal relativistic mass.
 
Last edited:
csmcmillion said:
"Relativity requires different values for the inertia of a moving object: in its direction of motion, and perpendicular to that direction. This contradicts the logical principle that the laws of physics are the same in all directions."

Are you quoting this from Conservapedia's "Counterexamples to Relativity" page?
 
jtbell said:
Are you quoting this from Conservapedia's "Counterexamples to Relativity" page?

Yes - that's where I found this. Supposedly, CP's founder has a BSEE from Princeton... (scratching head).
 
csmcmillion said:
Yes - that's where I found this. Supposedly, CP's founder has a BSEE from Princeton... (scratching head).

Well the idea of transverse and longitudinal relativistic mass is not clearly wrong. In fact, it is fairly common in old books. I would describe the evolution away from it as: if some definitions force such complexity, and other definitions that are at least as simple do not, let's avoid the definitions with adverse side effects.
 
In an inertial frame of reference (IFR), there are two fixed points, A and B, which share an entangled state $$ \frac{1}{\sqrt{2}}(|0>_A|1>_B+|1>_A|0>_B) $$ At point A, a measurement is made. The state then collapses to $$ |a>_A|b>_B, \{a,b\}=\{0,1\} $$ We assume that A has the state ##|a>_A## and B has ##|b>_B## simultaneously, i.e., when their synchronized clocks both read time T However, in other inertial frames, due to the relativity of simultaneity, the moment when B has ##|b>_B##...

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